WO2004098234A1

WO2004098234A1 - Ultrasonic sensor

Info

Publication number: WO2004098234A1
Application number: PCT/JP2003/005436
Authority: WO
Inventors: Masahiko Hashimoto; Hidetomo Nagahara; Masaaki Suzuki
Original assignee: Matsushita Electric Industrial Co., Ltd.
Priority date: 2003-04-28
Filing date: 2003-04-28
Publication date: 2004-11-11
Also published as: EP1610587B1; ATE513188T1; JP3722827B2; US20050139013A1; JPWO2004098234A1; EP1610587A1; US7162930B2; AU2003231547A1; CN1703929A; EP1610587A4

Abstract

An ultrasonic sensor comprising an ultrasonic vibrator (2) for transmitting and/or receiving an ultrasonic wave, and a propagation medium section (6) forming a propagation path of ultrasonic wave, wherein the mutual relation is set appropriately between the density ρ1 and the sound velocity C1 of the propagation medium section (6), and between the density ρ2 and the sound velocity C2 of fluid filling the surrounding space, and propagation loss of ultrasonic wave into the fluid is substantially reduced to zero by refracting the ultrasonic wave at an appropriate angle.

Description

Description Ultrasonic sensor Technical field

The present invention relates to an ultrasonic sensor for transmitting or receiving ultrasonic waves, more specifically, an ultrasonic transmitter for transmitting ultrasonic waves, or an ultrasonic receiver for receiving ultrasonic waves, or The present invention relates to an ultrasonic transducer that performs either or both of the forces. Background art

In recent years, ultrasonic transducers have been industrially used in a wide range of fields such as distance measurement, object detection, flow measurement, and robot control.

As the first ultrasonic transducer, for example, there is an ultrasonic transducer described in Japanese Patent Publication No. 6-180880. Hereinafter, the configuration and operation of a conventional ultrasonic transducer will be described with reference to FIG.

FIG. 10 is a cross-sectional view of a first conventional ultrasonic transducer. In FIG. 10, 100 indicates an ultrasonic transducer, 101 indicates an ultrasonic transducer, 102 indicates an acoustic matching layer, and 103 indicates a housing.

First, the operation at the time of transmitting waves in the configuration of FIG. 10 will be described. The ultrasonic transducer 101 is supplied with a drive signal from a drive circuit (transmitting circuit 701) via a signal line 104, and generally receives a drive signal of the ultrasonic transducer 101. Ultrasonic vibration is generated at a frequency near the resonance frequency. The ultrasonic vibration generated in the ultrasonic transducer 101 is transmitted to the fluid around the ultrasonic transducer via the acoustic matching layer 102. The acoustic matching layer 103 is made of a material having an acoustic impedance that is intermediate between the acoustic impedance of the surrounding fluid and the acoustic impedance of the ultrasonic transducer 101, and improves the efficiency of transmitting waves to the surrounding fluid. Has a function.

Ultrasonic vibrator 1 0 1 for generating ultrasonic vibrations, typically Irare use piezoelectric ceramics, its acoustic impedance, for example, in ^{3 0 X 1 0 6 kg ·} m- 2 · s one degree . When the surrounding fluid is a gas such as air, for example, the acoustic impedance of air The acoustic impedance of the acoustic matching layer 102 is set to about 0.11 X 10 ⁶ kg · m ” ² · s- ¹ ) and the thickness is about 400 kg kgm— ² ■ s—. Is preferably set to 1 Z4, which is the wavelength at the assumed ultrasonic frequency.Conventionally, since a matching layer having an intermediate acoustic impedance between a piezoelectric vibrator and air is formed, the density is relatively small. A material is used in which a material (eg, glass balloon / plastic balloon) is hardened with resin.

Next, the operation during ultrasonic wave reception will be described. The ultrasonic wave that has propagated in the surrounding fluid and has reached the ultrasonic transducer 100 is transmitted to the ultrasonic transducer 101 via the acoustic matching layer 102 in reverse to the ultrasonic wave transmission. The ultrasonic transducer 101 converts the mechanical action of the ultrasonic wave into an electric signal, and the signal is transmitted to an electric processing unit (not shown) via the signal line 104.

In the transmission / reception operation of the ultrasonic transducer 100 described above, the transmission / reception of ultrasonic waves is performed in the laminating direction of the ultrasonic transducer 101 and the acoustic matching layer 102, that is, in the direction perpendicular to the acoustic matching layer 102.

As the second conventional ultrasonic transducer, there is, for example, an ultrasonic transducer disclosed in Japanese Patent Application Laid-Open No. 2000-304581 in the form of an ultrasonic flowmeter. Hereinafter, the configuration and operation of a conventional ultrasonic transducer will be described with reference to FIG. FIG. 11 is a sectional view of a second conventional ultrasonic transducer. In FIG. 11, reference numeral 104 denotes a first acoustic matching layer, and reference numeral 105 denotes a second acoustic matching layer. The first acoustic matching layer 104 has a structure in which a plurality of material plates (104a, 104b, 104c, {circle over (1)}) having different sound velocities and densities are laminated, and the first acoustic matching layer 104 is laminated from a material having a higher sound velocity to a material having a smaller sound velocity.

Hereinafter, the operation of the ultrasonic transducer 100 in the configuration of FIG. 11 will be described. At the time of transmitting waves, the ultrasonic waves generated by the ultrasonic transducer 101 by the drive signal applied by a signal line (not shown) are applied to the first acoustic matching layer 104 (104a, 104b, 104). c · · ■) and is incident on the second acoustic matching layer 105. The ultrasonic waves pass through the respective layers (104a, 104b, 104c, ···) of the stacked first acoustic matching layer 104 so as to be equal, and the first acoustic matching layer 104 and the second acoustic matching layer 104 have the same time. At the interface of the acoustic matching layer 105, the wavefront of the ultrasonic wave coincides. That is, the second acoustic matching layer In 105, the light propagates in the direction perpendicular to the interface with the first matching layer 104.

The ultrasonic wave that has propagated in the second acoustic matching layer 105 is refracted by the difference in the speed of sound between the second acoustic matching layer 105 and the interface of the surrounding fluid, changes its direction, and is emitted to the surrounding fluid. . At the time of reception, the ultrasonic wave that has propagated the surrounding fluid and reached the ultrasonic transducer 100 in the reverse process to that of the transmission, is transmitted at the interface with the second acoustic matching layer 105. The light is refracted and incident on the second acoustic matching layer 105, and is converted into an electric signal by the ultrasonic transducer 101 via the first acoustic matching layer 104. In this case, the sound wave arriving from the transmitting direction is selectively received.

In the case of the second conventional ultrasonic transducer, the direction of the sound wave is changed using refraction, so when applying the ultrasonic transducer to an ultrasonic flowmeter, the ultrasonic transducer is used for the measurement flow path. Since it can be integrated with the wall, it has the advantage of not causing disturbance in the flow of the fluid to be measured.

However, even when a low-density matching layer such as the first conventional ultrasonic transducer is used, when ultrasonic waves are transmitted from an ultrasonic transducer such as a piezoelectric ceramic into a gas such as air, There was a problem that propagation loss inevitably occurred and the efficiency of transmission and reception decreased. The reason that it is difficult to efficiently transmit ultrasonic waves from a solid to a gas is that the acoustic impedance of a gas is much smaller than that of a solid, and even if a matching layer is interposed in the middle, the ultrasonic This is because strong reflection occurs. Further, in the ultrasonic transducer of the type in which the refraction shown in the second conventional ultrasonic transducer described above is used to deflect the ultrasonic wave, the loss accompanying the deflection angle is added and the deflection angle becomes large. There was the problem that the transmission and reception efficiency was extremely low and could not be practically applied. Accordingly, the present invention has been made in view of the above problems, and a purpose thereof is to provide a highly sensitive ultrasonic sensor capable of deflecting ultrasonic waves and having high transmission and reception efficiency. It is in. Disclosure of the invention

The present invention is configured as follows to achieve the above object.

The present invention relates to an ultrasonic sensor that transmits or receives ultrasonic waves to or from a surrounding space filled with a fluid, An ultrasonic transducer,

Provided is an ultrasonic sensor including a propagation medium portion that fills a space between the ultrasonic transducer and the surrounding space to form a propagation path of the ultrasonic wave.

The ultrasonic sensor by Ryoaki Honmei is an ultrasonic sensor that transmits or receives ultrasonic waves to or from the surrounding space filled with fluid.

An ultrasonic transducer,

A propagation medium portion disposed between the ultrasonic transducer and the surrounding space to form a propagation path of the ultrasonic wave;

The density P of the propagation medium portion P is the sound velocity C of the propagation medium portion C The density p _{2 of} the fluid filling the space and the sound speed C _{2 of the} fluid filling the space are (p ₂ / p <(C _x / C ₂ ) <1.

An ultrasonic sensor according to the present invention is an ultrasonic sensor that transmits or receives an ultrasonic wave to or from a surrounding space filled with a fluid,

An ultrasonic transducer,

A propagation medium portion disposed between the ultrasonic transducer and the surrounding space and forming a propagation path of the ultrasonic wave;

A reflector disposed in contact with the propagation medium to control the propagation path of the ultrasonic wave; a density P of the propagation medium; a sound velocity C in the propagation medium; C; a density p _{2 of} a fluid filling the space; acoustic velocity C ₂ in the fluid satisfying及Pi said space, configured to satisfy p. Roh p rather (cc ₂₎ Ku-one relationship.

According to the present invention, a flow measurement unit having an inner wall defining a flow path of a fluid to be measured is provided outside a flow path space surrounded by an inner wall of the flow measurement unit, and transmits or receives ultrasonic waves. Do at least one ultrasonic transducer,

A propagation medium portion disposed between the ultrasonic transducer and the flow path space and forming a propagation path of the ultrasonic wave;

An ultrasonic flowmeter having

The density _{P of the} propagation medium portion The sound velocity in the propagation medium portion. The density p _{2 of} the measured fluid and the sound velocity C _{2 of the} measured fluid are ₂ Z _{P l} ) <(C C ₂ ) Provide an ultrasonic flowmeter configured to satisfy the relationship of <1.

According to a twenty-seventh aspect of the present invention, a flow measuring unit having an inner wall defining a gas flow path,

A pair of ultrasonic vibrators provided outside the flow path space surrounded by the inner wall of the flow rate measuring unit and transmitting or receiving ultrasonic waves,

A pair of propagation medium portions disposed between each of the pair of ultrasonic transducers and the channel space, and refracting a propagation path of the ultrasonic wave;

With

The propagation medium portion has a first surface region facing the ultrasonic vibration surface of the ultrasonic transducer, and a second surface region facing the flow path space,

The first surface region of the propagation medium portion is inclined with respect to the flow direction of the gas in the flow path space, and the second surface region is inclined with respect to the flow direction of the gas in the flow path space. To provide an ultrasonic flow meter that is substantially parallel.

According to a twentieth aspect of the present invention, there is provided an ultrasonic sensor for transmitting or receiving ultrasonic waves to a surrounding space filled with a fluid,

An ultrasonic transducer,

A propagation medium portion that fills a space between the ultrasonic transducer and the surrounding space and forms a propagation path of the ultrasonic wave;

The propagation medium portion has a first surface region facing an ultrasonic vibration surface of the ultrasonic transducer and a second surface region facing a flow that fills the surrounding space. The second surface region provides an ultrasonic sensor that is inclined with respect to the first surface region. BRIEF DESCRIPTION OF THE FIGURES

These and other objects and features of the present invention will become apparent from the following description in connection with the preferred embodiments of the accompanying drawings. In this drawing,

FIG. 1A is a perspective view of an overview of an ultrasonic transducer according to a first embodiment of the present invention,

FIG.1B is a cross-sectional view of FIG.1A orthogonal to the longitudinal direction of the ultrasonic transducer of the first embodiment. B—A sectional view taken along line B,

FIG. 2 is a cross-sectional view showing the refraction of ultrasonic waves at the interface between the propagation medium part of the ultrasonic transducer and the fluid in the surrounding space.

FIG. 3A is a perspective view showing an overview of an ultrasonic transducer according to a second embodiment of the present invention, and FIG. 3B is a cross-sectional view of the ultrasonic transducer according to the second embodiment, taken along a cylindrical center line. FIG. 3C is a perspective view showing an example of the electrode structure of the ultrasonic transducer of the ultrasonic transducer according to the second embodiment,

FIG.4A is a perspective view of an overview of one ultrasonic transducer according to a third embodiment of the present invention,

FIG. 4B is a cross-sectional view of the ultrasonic transducer of FIG. 4A of the third embodiment, taken along a cylindrical center line,

FIG.5A is a perspective view of an overview of another ultrasonic transducer according to the third embodiment of the present invention,

FIG. 5B is a cross-sectional view of the ultrasonic transducer of FIG. 5A of the third embodiment, taken along a cylindrical center line,

FIG. 6A is a perspective view showing an overview of an ultrasonic transducer according to a fourth embodiment of the present invention,

FIG. 6B is a cross-sectional view of the ultrasonic transducer of the fourth embodiment on the cylindrical center line, and FIG. 6C is a center axis of another cylindrical ultrasonic transducer of the fourth embodiment. FIG.

FIG.6D is a perspective view showing an example of an electrode surface of an ultrasonic transducer of the ultrasonic transducer according to the fourth embodiment,

FIG. 7 is a partial cross-sectional perspective view of an ultrasonic handset according to a fifth embodiment of the present invention. FIGS. 8A and 8B are schematic views of an ultrasonic handset according to a sixth embodiment of the present invention. FIGS. 9A, 9B, and 9C are explanatory diagrams when the ultrasonic handset according to the seventh embodiment of the present invention is applied to different fields, respectively.

FIG. 10 is a cross-sectional view of a conventional ultrasonic transducer.

FIG. 11 is a cross-sectional view of another conventional ultrasonic transducer.

FIGS. 12A and 12B show the longitudinal direction of the ultrasonic flowmeter according to the eighth embodiment of the present invention. FIG. 12B is a cross-sectional view taken along the line BB of FIG. 12A, which is orthogonal to the longitudinal direction of the ultrasonic flowmeter according to the eighth embodiment;

FIG. 13 is a diagram showing the refraction of ultrasonic waves at the interface between the propagation medium and the fluid to be measured.

FIG. 14 is a sectional view of an ultrasonic flowmeter according to the ninth embodiment of the present invention. FIGS. 15A, 15B, and 15C show modified examples of the eighth and ninth embodiments of the present invention. FIG. 2 is a cross-sectional view of such an ultrasonic flowmeter,

FIGS. 16A and 16B are cross-sectional views of ultrasonic flow meters according to other modified examples of the eighth and ninth embodiments of the present invention.

FIG. 17 is a cross-sectional view of a conventional ultrasonic flowmeter. BEST MODE FOR CARRYING OUT THE INVENTION

Before continuing the description of the present invention, the same parts are denoted by the same reference numerals in the accompanying drawings.

Hereinafter, preferred embodiments of the present invention will be described with reference to the drawings, but before that, various aspects of the present invention will be described.

According to a first aspect of the present invention, there is provided an ultrasonic sensor for transmitting or receiving ultrasonic waves to a surrounding space filled with a fluid,

An ultrasonic transducer,

According to a second aspect of the present invention, there is provided an ultrasonic sensor for transmitting or receiving an ultrasonic wave with respect to a surrounding space filled with a fluid,

An ultrasonic transducer,

The density P of the above-mentioned propagation medium portion is the sound velocity C of the above-mentioned propagation medium portion.The density p _{2 of} the fluid that fills the above space, and the sound velocity C _{2 of the} fluid that fills the above space are (p ₂ / p,) <(C , / C ₂ ) to provide an ultrasonic sensor configured to satisfy the relationship of (1) You.

According to a ^third aspect of the present invention, the propagation medium portion includes: a first surface region facing the ultrasonic vibration surface of the ultrasonic vibrator; and a second surface region facing the flow that fills the surrounding space. The ultrasonic sensor according to the second aspect, wherein the second surface region of the propagation medium portion is inclined with respect to the first surface region.

According to a fourth aspect of the present invention, there is provided an ultrasonic sensor for transmitting or receiving ultrasonic waves to a surrounding space filled with a fluid,

An ultrasonic transducer,

A reflector that is disposed in contact with the propagation medium portion and controls a propagation path of the ultrasonic wave,

The density P of the propagation medium part is the sound velocity c of the propagation medium part.The density of the fluid filling the space Ρ ₂ , and the sound velocity C _{2 of the} fluid filling the space is (p ₂ / p) <(c ₂ ) Provide an ultrasonic sensor configured to satisfy the relationship of <1.

According to the fifth aspect of the present invention, the propagation medium portion includes: a first surface region facing the ultrasonic vibration surface of the ultrasonic vibrator; and a second surface region facing the flow filling the surrounding space. And at least one third surface region disposed between the first surface region and the second surface region of the ultrasonic wave propagation path and in contact with the reflector. The ultrasonic sensor according to the fourth aspect, wherein the second surface region is inclined with respect to at least one of the first surface region and the third surface region.

According to the sixth aspect of the present invention, the incident angle θ _{1 of the} ultrasonic wave to the interface between the propagation medium portion and the fluid filling the surrounding space, the density p of the propagation medium portion, the fluid filling the surrounding space, density p _2, and the approach angle theta ₂ of the ultra-sound waves from the interface to the fluid filling the surrounding space,

The ultrasonic sensor according to any one of the first to fifth aspects, wherein the ultrasonic sensor is configured to substantially satisfy the relationship of ot S sZ cote. According to a seventh aspect of the present invention, the propagation medium portion is made of an inorganic oxide or an organic polymer. An ultrasonic sensor according to any one of the first to fifth aspects, wherein the ultrasonic sensor is formed from a dried gel.

According to an eighth aspect of the present invention, there is provided the ultrasonic transmission sensor according to the sixth aspect, wherein the solid skeleton of the dried gel is hydrophobized.

According to a ninth aspect of the present invention, the density of the dried gelle is 500 kg Zm ³ or less, and the average pore diameter of the dried gel is 100 nm or less. An ultrasonic sensor is provided.

According to a tenth aspect of the present invention, there is provided an acoustic matching layer provided between the ultrasonic vibrator and the propagation medium section for acoustically matching the ultrasonic vibrator and the propagation medium section. The ultrasonic sensor according to any one of the first to fifth aspects has the following. According to a first aspect of the present宪明, fluid filling the surrounding space, ultrasound according to any one aspect of the 1-5 density p ₂ is 1 0 kg / m ³ or less of the gas Provide a sensor.

According to the 12th aspect of the present invention, the ultrasonic sensor according to any one of the first to 5th aspects, wherein the transmitting or receiving direction of the ultrasonic wave is substantially parallel to the second surface region. I will provide a.

Hereinafter, embodiments of the present invention will be described in detail.

(First Embodiment)

Hereinafter, an ultrasonic transducer as an example of the ultrasonic sensor according to the first embodiment of the present invention will be described in detail with reference to the drawings.

The present inventor has found that, in an ultrasonic transducer, if ultrasonic waves are appropriately refracted by using a propagation medium made of an appropriate material, almost no loss occurs at the interface, and solids to fluids (particularly gas The inventors have found that ultrasonic waves can be propagated to the present invention, and have arrived at the present invention.

In the ultrasonic transducer according to the first embodiment of the present invention, the surface parallel to the vibration surface of the ultrasonic vibrator (the first surface region) and the surface (the second surface region) in contact with the fluid filling the surrounding space are provided. ) Is disposed between the ultrasonic transducer and the fluid filling the surrounding space. In the description and claims of the present application, “fluid filling the surrounding space” means a fluid at least in contact with the second surface region, and is not necessarily an ultrasonic transmission sensor. It does not mean a fluid that fills the entire surroundings (for example, an ultrasonic transducer), but a fluid that fills a part of the surroundings.

First, an ultrasonic transducer according to a first embodiment of the present invention will be described with reference to FIGS. 1A and 1B. FIG. 1A is a perspective view of an outline of the ultrasonic transducer 1 according to the first embodiment, and FIG. 1B is a cross-sectional view of the ultrasonic transducer 1 along BB ′ in FIG. 1A. FIG.

The ultrasonic transducer 1 shown in FIGS. 1A and 1B includes an ultrasonic transducer 2 that converts an electric signal into ultrasonic vibration or converts ultrasonic vibration into an electric signal, and a fluid in the surrounding space. A propagation medium portion 6 disposed between the ultrasonic transducer 2 and the ultrasonic transducer 2 to form a propagation path of the ultrasonic wave; and a propagation medium disposed between the ultrasonic transducer 2 and the propagation medium portion 6 to propagate the ultrasonic wave. An acoustic matching layer 3 for matching the acoustic impedance of the medium section 6, a vibrator case section 4 containing the ultrasonic vibrator 2 and also serving as an electrical conduction path with the ultrasonic vibrator 2, and a terminal plate 9X And two signal lines 5 for inputting / outputting signals to / from the ultrasonic vibrator 2 and a part of the two signal lines 5 to prevent an electrical short between the two signal lines 5 And a housing 9 for accommodating the ultrasonic vibrator 2, the propagation medium 6, the acoustic matching layer 3, and the vibrator case 4. As shown in FIGS. 1A and 1B, the housing 9 is fixed to a cylindrical side portion 9 y cut so as to be inclined at a predetermined angle with respect to the axial direction, and is fixed to the bottom of the side portion 9 y. And a terminal plate 9X functioning as a part of the terminal board 9.

The propagation medium portion 6 is a space surrounded by the housing 9 defined by the terminal plate 9X and the side portion 9y, and a space outside the oscillator case portion 4 and other than the acoustic matching layer 3 disposed in the space. And the first surface region 7 facing the acoustic matching layer 3 and the ultrasonic transducer 2 (but directly facing the acoustic matching layer 3) and the first surface region 7 facing the fluid filling the surrounding space. And two surface regions 8. Further, the second surface region 8 of the propagation medium portion 6 is inclined by a predetermined angle so as not to be parallel to the first surface region 7. Here, the predetermined angle is, for example, an angle larger than 0 ° and smaller than 90 °, but is preferably substantially smaller than 80 °. In the first embodiment, the density of the fluid density and sound velocity of _P had the propagation medium portion 6 of the propagation medium portion 6 satisfies the C ₁ surrounding space was p _2, the acoustic velocity of the fluid filling the surrounding space and C ₂ At this time, the material of the propagation medium 6 is selected so that the relationship shown in the following equation (1) is satisfied.

(p ₂ / p _x ) <(C / C ₂ ) <1 (1) If the fluid is a gas such as air, it is difficult to find a material that satisfies the above conditions. The reason is that the sound velocity than the acoustic velocity C ₂ gases is because small solid material is small. In the first embodiment, the propagation medium section 6 is formed from a dried gel of an inorganic oxide or an organic polymer in order to realize the propagation medium section 6 that satisfies the above conditions. The solid skeleton of the dried gel used in the first embodiment is hydrophobized, and has a density of 500 kg / m ³ or less. This dry gel is a nanoporous dry gel having an average pore diameter of 100 nm or less (nanoporous dry gel).

The solid skeleton of the dried gel of inorganic oxide preferably contains at least silicon oxide (silicon) or aluminum oxide (alumina) as a component. The solid skeleton of the dried gel of the organic polymer can be made of a general thermosetting resin or thermoplastic resin. For example, polyurethane, polyurea, phenol-cured resin, polyatarylamide, polymethylmethacrylate, or the like can be used.

When the propagation medium section 6 is formed of, for example, a nanoporous dry gel containing silica as a main component, if the density p is 200 kg / m ³ , the sound velocity can be changed from 10 OmZs to 180 m / s. It can be set in the range of about. If fluid filling the surrounding space is air, the density p ₂ of air is 1. 2 2 kg / m ^3, the acoustic velocity C ₂ is 34 Om / s der Runode, by employing the propagation medium portion 6 of the , P sp and C _a <C 2 at the same time, and the force, (p ₂ / _{P l} ) <

This relationship can be satisfied. When measuring a gas such as natural gas, the propagation medium section 6 preferably has a density p of 100 to 300 kg / m ³ and a sound velocity of 100 to 30 Om / s.

The ultrasonic vibrator 2 is a piezoelectric body, and can generate an ultrasonic vibration and / or an electric signal by the application of an electric signal. As the piezoelectric body, a piezoelectric ceramic is preferably used. In cases where the resonance characteristics are controlled and the mechanical Q value is reduced, an absorber may be placed around the case. In the ultrasonic transducer 1 of the first embodiment, the acoustic matching layer 3 is provided between the propagation medium 6 and the ultrasonic vibrator 2, and the ultrasonic wave is transmitted to the ultrasonic vibrator 2 as an ultrasonic wave generating source. It has a function of enhancing acoustic matching with the medium section 6.

Nanoporous dry gel mainly composed of silica '(acoustic Inpidansu ^{3 X 1 0 4 kg ■ m-} 2 · s - 1)) to form a force et propagation medium portion 6, the force, one ultrasonic transducer 1 There piezoelectric ceramics (acoustic ^{impedance: 3 0 X 1 0 6 kg} ■ m- 2 ■ s "1)) when configured for one acoustic Inpidansu ^{^{X 1 0 6 kg - m- 2}} ■ s ^-1 ) By adopting the acoustic matching layer 3 made of a material in the vicinity, the propagation efficiency of the ultrasonic energy can be made approximately 1, specifically, 0.95 or more. It can be realized by a composite material in which hollow glass spheres are solidified with a resin material, or a porous ceramic The thickness of the acoustic matching layer 3 is preferably set to 1/4 wavelength of the ultrasonic wave to be used. In the ultrasonic transducer 1 of the embodiment, the ultrasonic vibrator 2 is contained in the vibrator ′ case 4. The transducer 2 is joined to the inside of the top of the transducer case 4 and the acoustic matching layer 3 is joined to the outside of the top of the transducer case 4 to form a laminated structure.The transducer case 4 is preferably made of a conductive material such as stainless steel. The thickness between the ultrasonic vibrator 2 and the acoustic matching layer 3 is set to 1/10 or less, and preferably 1/20 or less, of the assumed ultrasonic wavelength. Acoustic matching can be maintained in a good state.

The vibrator case 4 is joined to the terminal plate 9X of the housing 9 by a method such as electric welding, and can have a sealed structure in which an inert gas such as dry nitrogen or argon is injected. With the above configuration, the ultrasonic vibrator 2 is physically isolated from the outside air environment and can achieve improved reliability, and also has an electrically shielded structure. High safety can be ensured even when the fluid is flammable.

Next, how the ultrasonic wave propagates from the propagation medium 6 to the fluid filling the surrounding space will be described in detail with reference to FIG.

From the arrangement described above, since the ultrasonic wave is incident from the normal direction of the first surface region 7 which is facing and parallel to the vibration surface of the ultrasonic vibrator 1, the ultrasonic wave and the fluid filling the surrounding space Along the direction inclined from the normal direction of the second surface region 8 which is the interface of Ultrasonic waves enter. The incident angle of the ultrasonic wave with respect to the normal direction of the second surface region 8 is Θi (0 ° eg cT). At this time, the ultrasonic wave is refracted at the second surface region 8 which is the interface between the propagation medium portion 6 and the fluid filling the surrounding space, and enters the fluid to be measured at an angle (entrance angle) θ ₂ with respect to the normal direction. (Θ, <θ ₂ ).

In the first embodiment described above, given the density ρ _{2 of the} fluid filling the surrounding space, various parameters Θ and Θ ₂ ) are set so as to substantially satisfy the relationship of the following equation (2). ing.

(ρ ₂ / Ρ!) = (cot 0 ₂ / cot θ (2) With such a setting, the propagation efficiency of the ultrasonic energy from the propagation medium 6 to the fluid filling the surrounding space becomes almost 1. Then, the incident angle 0 satisfies the condition expressed by the following equation (3).

(cot) ² =

_{_{^{[(C l Xc 2) 2}}} - 1] / [(p 2 / P l) 2 - (c Bruno c ₂₎ ^2]

(3) Accordingly, if p ₁ and C _{2 of} the propagation medium 6 and p ₂ and C _{2 of the} fluid filling the surrounding space are determined, the angle of incidence 0 is determined by equation (3). If the incident angle is determined, the approach angle 0 ₂ is also determined by equation (2). Once the incident angle 6 and the approach angle θ ₂ are determined, the inclination angle of the second surface region 8 of the propagation medium 6 and the like can also be determined. More than that, even in the case of reception of ultrasonic waves propagated through the fluid filling the surrounding space because it is directly applied, the ultrasonic waves coming from the direction of approach angle 0 ₂ is selectively received wave.

In the first embodiment, by forming the propagation medium section 6 from the above-described material, the sound velocity Ci of the propagation medium section 6 can be set to 18 Om / s, and the density p can be set to 200 kgZm ³ . When the surrounding space is a normal space filled with air, the air density p 2 is 1.22 kg / m ³ and the sound velocity C ₂ is 34 Om / s.

The relationship (3), the angle of incidence 3 2 °, the approach angle 0 ₂ may be set to 89 °. Since the approach angle 0 ₂ is close to 90 °, the ultrasonic wave transmitted into the air travels substantially parallel to the second surface region 8 that is the transmitting surface. Therefore, the transmission and reception direction of the sound wave of the first embodiment is defined by the line BB ′ in the plane including the second surface region 8 shown in FIG. 1A. Along the direction of arrow 90 in FIG. 1A.

According to the first embodiment, since propagation loss hardly occurs in the second surface region 8, which is the interface between the propagation medium portion 6 and the fluid filling the surrounding space, the two acoustic impedances are matched at this interface. No need. Therefore, the ultrasonic waves emitted from inside the propagation medium portion 6 are refracted at the second surface region 8 which is the interface between the propagation medium portion 6 and the fluid filling the surrounding space, and are reflected along the plane including the second surface region 8. Since ultrasonic waves can be deflected in the directions and propagation loss hardly occurs in the second surface region 8, it is possible to provide a high-sensitivity ultrasonic sensor having high transmission and reception efficiency.

The propagation medium portion 6 does not need to be made of a material having a uniform density and sound velocity over the whole, and has a laminated structure in which a plurality of types of material layers having different densities pi and sound speeds C are stacked. May be. In the case of having such a laminated structure, the ultrasonic wave may not travel straight through the propagation medium part 6, but there is no particular problem. The important point is that the density _{P, the} sound velocity, and the incident angle ΘS of the propagation medium 6 are set in the region near the interface between the propagation medium 6 and the fluid to be measured so as to satisfy the above expression. Next, the operation of the ultrasonic transducer in the first embodiment will be described.

First, when transmitting waves to a fluid that fills the surrounding space, the ultrasonic transducer 2 (8 in FIG. 9C) is transmitted from the transmission circuit 701, which also serves as the drive circuit, as shown in FIG. relative to 1), the resonant frequency near (e.g. 1 0 0 k H z~: AC voltage having a frequency of L approximately MH _Z), the pulse voltage, a burst voltage is applied. As a result, the ultrasonic vibrator 2 is excited to vibrate in the vicinity of the resonance frequency, and the vibration is radiated as ultrasonic waves to the propagation medium 6 through the vibrator case 4 and the acoustic matching layer 3 at a condition of approximately 1 efficiency. The sound wave propagating through the propagation medium section 6 is refracted at the second surface region 8 which is the interface between the propagation medium section 6 and the fluid filling the surrounding space, and is radiated to the fluid filling the surrounding space at a state of approximately 1 in efficiency.

Next, when receiving the ultrasonic wave that propagates through the fluid filling the surrounding space and reaches the ultrasonic transducer 1, the path of the ultrasonic wave propagating from the transmitting direction is the reverse of the case of transmitting the ultrasonic wave. The ultrasonic wave incident on the ultrasonic transducer 1 arrives at the ultrasonic vibrator 2 under the condition of almost efficiency 1, is converted into an electric signal, and is converted into an electric signal through an external electric circuit (for example, a receiving circuit). 7 0 2). According to the first embodiment, the propagation medium portion 6 displaying appropriate density p and velocity of sound C _x provided to refract an ultrasonic wave to an appropriate angle, and substantially zero propagation loss at the interface of the material, good Flow measurement can be achieved with SZN ratio. According to the first embodiment, the ultrasonic wave is appropriately refracted by using the propagation medium section 6 and almost no loss occurs at the interface. Since it is possible to transmit and receive ultrasonic waves of gases (for example, hydrogen gas) that were extremely difficult to transmit and receive, application to flow measurement and the like that can measure these gases becomes possible.

Furthermore, in the ultrasonic transducer 1 according to the first embodiment, the ultrasonic waves emitted from the inside of the propagation medium portion ⁶ emit the second surface area 8 which is the interface between the propagation medium portion 6 and the fluid filling the surrounding space. The transmission and reception direction of the ultrasonic wave is deflected in the direction along the plane including the second surface region 8, so that, for example, in a flow meter, the measurement flow path has no irregularities related to the mounting of the transducer, and the fluid A flow meter without flow disturbance can be constructed. Even if it is mounted in alignment with the horizontal plane of various devices having a horizontal part, it can be applied to the detection of objects in the horizontal direction.

(Second embodiment)

An ultrasonic transducer as an example of the ultrasonic sensor according to the second embodiment of the present invention will be described with reference to FIGS. 3A, 3B, and 3C. 3A is a perspective view of the appearance of the ultrasonic transducer 11 in the second embodiment, FIG. 3B is a cross-sectional view including the central axis of the cylindrical ultrasonic transducer 11, and FIG. FIG. 3 is a perspective view showing an example of an electrode structure of the ultrasonic transducer 12. The same reference numerals are given to members common to the second embodiment and the first embodiment. The propagation medium 6A corresponds to the propagation medium 6 of the first embodiment, and the housing 9A corresponds to the housing 9 of the first embodiment.

Hereinafter, features of the ultrasonic transducer 11 according to the second embodiment will be described, and description of the same parts as those of the ultrasonic transducer 1 according to the first embodiment and the corresponding parts will be omitted. .

Ultrasonic transducer 1 1 of the second embodiment is the side 9 _Z cylindrical shape is fixed to the terminal plate 9 X disc-shaped is composed of a housing 9 A, the center of the terminal plate 9 X It is configured axisymmetrically around a fixed central axis 9a. Therefore, housing 9 The supersonic transducer 12 and the acoustic matching layer 13 arranged on the disk-shaped terminal plate 9x of A are formed in a ring shape. Further, a disk-shaped protection portion 15 having a central portion joined to the central shaft 9a, which is a part of the housing 9A, is further provided to protect the second surface area 8, and the housing 9A and the protection portion 1 are protected. A ring-shaped opening 14 is provided between 5 and ultrasonic waves are transmitted and received through the opening 14 in the direction of arrow 9OA. The space in the housing 9A and the space other than the supersonic transducer 12 and the acoustic matching layer 13 is almost filled with the propagation medium 6A. The propagation medium portion 6A faces the acoustic matching layer 13 and the ultrasonic transducer 12 (however, directly faces the acoustic matching layer 13), the first surface region 7 and the surrounding space. And a second surface region 8 facing the fluid that satisfies the following conditions. Furthermore, the second surface region 8 of the propagation medium portion 6A is substantially evenly directed from the periphery to the center side with respect to the center axis 9a so as not to be parallel to the first surface region 7. Is inclined by a predetermined angle.

In the second embodiment, specific transmission and reception of ultrasonic waves are performed with high efficiency as in the first embodiment, and the same effects as in the first embodiment can be obtained. The difference from the first embodiment is that the ultrasonic transducer 11 has an axially symmetric structure around the central axis 9a, and can transmit and receive waves in all directions around the central axis 9a. This is a structural point. When the surrounding space is a gas, the transmitted and received waves are almost horizontal, and application to omnidirectional object sensing is possible.

FIG. 3C shows an example of the electrode structure of the ultrasonic transducer 12, and 16 is a divided electrode portion formed on the electrode surface. By dividing the electrode section 16 as shown in Fig. 3C, the vibration generation section can be controlled, so that scanning by ultrasonic waves in the circumferential direction becomes possible, and application to object detection in a specified direction is possible. Will be possible.

The electrode portion may be divided on at least one surface of the electrode portion 16 formed on the front and rear sides, and the same effect can be obtained by dividing and arranging the ultrasonic transducer 12 itself. In FIG. 3C, the number of divisions of the electrode section 6 is 4, but the number of divisions is arbitrary, and it is not necessarily required to be the same or symmetric.

(Third embodiment)

An ultrasonic transducer as an example of the ultrasonic sensor according to the third embodiment of the present invention will be described with reference to FIGS. 4A and 4B and FIGS. 5A and 5B. Figure 4A shows the third FIG. 4B is a perspective view of the appearance of the ultrasonic transducer 21 in the embodiment, and FIG. 4B shows a cross section including the center axis of the cylindrical ultrasonic transducer 21. FIG. 5A is a perspective view of the appearance of another ultrasonic transducer 31 in the third embodiment, and FIG. 5B is a view showing the center axis 9 b of the cylindrical ultrasonic transducer 31. FIG. The same reference numerals are given to members common between the third embodiment and the above-described first and second embodiments. The propagation medium portions 6B and 6C correspond to the propagation medium portion 6 or 6A of the above embodiment, and the housings 9B and 9C correspond to the housing 9 or 9A of the above embodiment.

Hereinafter, features of the ultrasonic transducer 21 and the ultrasonic transducer 31 of the third embodiment will be described, and the ultrasonic transducer 1 and the second embodiment of the first embodiment will be described. The description of the same parts as those of the ultrasonic transducer 11 of the embodiment and the corresponding parts will be omitted.

As shown in FIGS. 4A and 4B, the housing 9B of the ultrasonic transducer 21 of the third embodiment has a terminal plate 9X fixed to a lower end of a cylindrical side portion 9g. A disc-shaped upper plate 9h having a circular opening 24 in the center is fixed to the upper end of the portion 9g, and the housing 9B is configured to be axially symmetric around the virtual center axis. The supersonic transducer 22 and the acoustic matching layer 23 fixed to the inner surface of the side 9 g of the housing 9B are formed in a cylindrical shape. Also, the propagation medium portion 6B is housed in the housing 9B so that the propagation medium portion 6B does not protrude inward from the center opening 24 of the disc-shaped upper plate 9b of the housing 9B. To protect the second surface area 8 with the entire housing 9B, and transmit and receive ultrasonic waves in the direction of the arrow 90B through the central opening 24 of the upper plate 9b of the housing 9B. . That is, the propagation medium portion 6B is filled in a space other than the supersonic transducer 22 and the acoustic matching layer 23 and the central portion arranged in the housing 9B. The propagation medium portion 6B faces the acoustic matching layer 23 and the ultrasonic vibrator 22 (however, directly faces the acoustic matching layer 23), and the first surface region 7 and the surrounding space. (In FIG. 4B, facing the space in the center). Further, the second surface region 8 of the propagation medium portion 6B extends from the upper end to the lower end substantially uniformly with respect to the central axis so as not to be parallel to the first surface region 7. Thus, a conical surface is formed by inclining by a predetermined angle. On the other hand, as shown in FIGS. 5A and 5B, the housing 9C of another ultrasonic transducer 31 of the third embodiment has a terminal plate 9X at the lower end of the cylindrical side portion 35. The center of the disc-shaped upper plate 9i is fixed to the center axis 9b fixed to the center of the terminal plate 9X, and the housing 9C is configured to be axially symmetric around the center axis 9b. Have been. The supersonic transducer 32 and the acoustic matching layer 33 fixed around the central axis 9b are formed in a cylindrical shape. Further, the propagation medium portion 6C is housed and arranged in the housing 9C so that the propagation medium portion 6C does not protrude outward from the periphery of the upper plate 9i of the housing 9C. 9 Protect the second surface area 8 with the protection part 35, which is a cylindrical side fixed to X, and provide a ring-shaped opening 34 between the housing 9C and the protection part 35, and the opening Transmission and reception of ultrasonic waves are performed in the direction of arrow 90 C through 34. In other words, the space other than the supersonic transducer 32, the acoustic matching layer 33, and the surroundings arranged in the housing 9C is filled with the propagation medium 6C. The propagation medium portion 6 C faces the acoustic matching layer 33 and the ultrasonic vibrator 32 (however, directly faces the acoustic matching layer 33), the first surface region 7, and the surrounding space. (In FIG. 5B, facing the surrounding space). Further, the second surface region 8 of the transfer medium portion 6C is spread almost uniformly from the lower end to the upper end with respect to the central axis so as not to be parallel to the first surface region 7. In addition, it is inclined by a predetermined angle to form a conical surface.

In the third embodiment, specific transmission and reception of ultrasonic waves are performed with high efficiency similarly to the first embodiment and the second embodiment, and the first embodiment and the second embodiment The same effect as described above can be obtained. The difference from the second embodiment is that ultrasonic waves are transmitted and received in the front direction of ultrasonic transducers 21 and 31 (upward in FIGS. 4B and 5B). The application of the existing ultrasonic transducer is possible.

(Fourth embodiment)

An ultrasonic transducer as an example of the ultrasonic sensor according to the fourth embodiment of the present invention will be described with reference to FIGS. 6A, 6B, 6C, and 6D. FIG. 6A is a perspective view of the appearance of the ultrasonic transducer 41 and the ultrasonic transducer 51 in the fourth embodiment, and FIG. 6B is a central axis of the cylindrical ultrasonic transducer 41. FIG. 6C is a cross-sectional view including the center axis of another cylindrical ultrasonic transducer 51 according to the fourth embodiment. FIG. 6D is a perspective view of an example of the electrode surfaces of the ultrasonic transducers 42 and 52 of the ultrasonic transducer according to the fourth embodiment. The same reference numerals are given to members common to the fourth embodiment and the first to third embodiments. The propagation medium portions 6D and 6E correspond to the propagation medium portion 6 or 6A of the previous embodiment, and the housings 9D and 9E correspond to the housing 9 or 9A of the previous embodiment.

Hereinafter, features of the ultrasonic transducer 41 and the ultrasonic transducer 51 of the fourth embodiment will be described, and the ultrasonic transducer 1 and the second embodiment of the first embodiment will be described. The description of the same parts as those of the ultrasonic transducers 11 and 21 in the form and the corresponding parts will be omitted.

As shown in FIGS. 6A and 6B, the housing 9D of the ultrasonic transducer 41 according to the fourth embodiment has a terminal plate 9X fixed to the lower end of the cylindrical side portion 9g. A frusto-conical reflector 44 is fixed to the center of the plate 9X, and a housing 9D is configured to be axially symmetric around the central axis of the reflector 44. The ultrasonic transducer 42 and the acoustic matching layer 43 fixed to the side 9 g of the housing 9 D and the inner surface of the terminal plate 9 X are cylindrical, and are acoustically matched inside the ultrasonic transducer 42. Layers 43 are arranged. The propagation medium 6D is accommodated in the housing 9D so that the propagation medium 6D does not protrude from the upper end surface of the reflector 44 of the housing 9D and the upper end surface of the side 9g. ing. Their to propagation medium portion 6 D has a first surface region 7 parallel to the plane of vibration of the ultrasonic vibrator ^{4 2,} and a second surface region 8 in contact with fluid filling the surrounding space, and the propagation medium The reflector 44 provided adjacent to the portion 6D is in contact with the third surface region 45.

The reflector 44 is made of a metal material such as stainless steel, and when the propagation medium portion 6 is formed of, for example, a dry nanoporous gel mainly composed of a sily force, the reflector 44 has a third surface region 45. The reflection efficiency becomes almost 1. The reflector 44 has an inclination angle set with respect to the first surface region 7 and the second surface region 8 so that the incident angle of the ultrasonic wave to the second surface region 8 satisfies Expression (3).

The ultrasonic vibrator 42 is excited by vibration near the resonance frequency, and the vibration is radiated as ultrasonic waves to the approximate center side of the propagation medium 6D through the acoustic matching layer 43 with a condition of approximately 1 efficiency. The sound wave propagating through the propagation medium portion 6D is reflected at the third surface area 45, which is the interface with the reflector 44, with almost efficiency 1, and the direction is changed to the second surface area 8 side. Then, the light is refracted at the second surface region 8, which is the interface between the propagation medium portion 6D and the fluid filling the surrounding space, and is emitted to the fluid filling the surrounding space at a state of approximately 1 in efficiency.

In addition, when an ultrasonic wave propagating in a fluid filling the surrounding space and arriving at the ultrasonic transducer 41 is received, the ultrasonic wave propagating from the transmission direction is opposite to the case of the transmission. The path is established, and the ultrasonic wave that has entered the second surface region 8 of the ultrasonic transducer 41 with almost efficiency 1 propagates through the propagation medium portion 6D and becomes the third interface at the interface with the reflector 44. The light is reflected at the surface area 45 under almost the condition of efficiency 1, and the direction of the light is substantially changed to the ultrasonic vibrator 42 and propagates, reaches the ultrasonic vibrator 42, and is generated by the ultrasonic vibrator 42. Converted to a signal.

With the above-described configuration, the ultrasonic transducer 41 can transmit and receive ultrasonic waves with high efficiency to a fluid that fills the surrounding space, and can provide the same effects as those of the first embodiment.

On the other hand, as shown in FIGS. 6A and 6C, the housing 9E of another ultrasonic transducer 51 of the fourth embodiment has a cylindrical reflector 54 having a triangular cross section. A terminal plate 9X is fixed to the lower end, a cylindrical central axis 9k is fixed to the center of the terminal plate 9X, and a disk-shaped upper plate 9m is like a flange at the upper end of the central axis 9k. The housing 9E is protruded and fixed, and the housing 9E is configured to be axially symmetric around the central axis of the reflector 54. The supersonic transducer 52 and the acoustic matching layer 53 fixed to the inner surface of the center axis 9 k of the housing 9 E, the upper plate 9 m, and the terminal plate 9 x are cylindrical, and the ultrasonic transducer 5 An acoustic matching layer 53 is disposed outside of 2. The propagation medium 6 is housed in the housing 9E so that the propagation medium 6E does not protrude beyond the upper end surface of the reflector 54 of the housing 9E and the upper end surface of the upper plate 9m. The propagation medium portion 6E has a first surface region 7 parallel to the vibration surface of the ultrasonic oscillator 52 and a second surface region 8 in contact with the fluid filling the surrounding space. The reflector 54 provided adjacent to 6E is in contact with the third surface region 55. The reflector 54 has the same material and the same inclination angle as the reflector 44.

The ultrasonic vibrator 52 is excited by vibration near the resonance frequency, and this vibration is radiated as ultrasonic waves to the substantially surrounding side of the propagation medium portion 6E under the condition of approximately 1 efficiency through the acoustic matching layer 53. The ultrasonic wave that has propagated through the propagation medium 6 E is the third ultrasonic wave at the interface with the reflector 54. The light is reflected at the surface area 5 with almost efficiency 1, and its direction is changed to the side of the second surface area 8 to propagate.The second surface area is an interface between the propagation medium 6E and the fluid filling the surrounding space. It is refracted at 8, and is emitted to the fluid that fills the surrounding space with almost efficiency 1.

In addition, when receiving an ultrasonic wave that propagates in a fluid filling the surrounding space and reaches the ultrasonic transducer 51, the ultrasonic wave propagating from the transmission direction is opposite to the case of the transmission. The path is established, and the ultrasonic wave incident on the second surface region 8 of the ultrasonic transducer 51 with almost efficiency 1 propagates through the propagation medium portion 6E, and becomes the third interface at the interface with the reflector 54. The light is reflected by the surface area 55 under the condition of the efficiency of approximately 1, and its direction is changed to the ultrasonic vibrator 52 side, propagates, reaches the ultrasonic vibrator 52, and is electrically generated by the ultrasonic vibrator 52. Converted to a signal.

With the above-described configuration, the ultrasonic transducer 51 can transmit and receive ultrasonic waves with high efficiency to a fluid that fills the surrounding space, and can provide the same effects as the first embodiment.

Note that a plurality of reflectors 44 and 54 of the fourth embodiment may be arranged, and in such a case, a plurality of third surface regions 45 and 55 are provided. Further, in this case, a configuration in which the first surface region 7 and the second surface region 8 are parallel to each other is also established, and at least one of the plurality of third surface regions 45, 55 is at least one of It is only necessary to incline at a predetermined angle.

The ultrasonic transducer 41 and the ultrasonic transducer 51 have a structure capable of transmitting and receiving signals in all directions around the central axis, similarly to the second embodiment, and when the surrounding space is a gas. In the meantime, the transmitted and received waves are almost horizontal, and it can be applied to object detection in all directions. Fig. 6D shows an example of the electrode structure of the ultrasonic vibrators 42 and 52, and 46 is a divided electrode formed on the inner surface of the cylindrical ultrasonic vibrators 42 and 52. Yes, 47 is a common electrode formed on the outer surface. By dividing the electrode part 46 as shown in Fig. 6D, the vibration generator can be controlled, so that it is possible to scan by ultrasonic waves in the circumferential direction, and it is possible to apply it to object detection in a specified direction. become.

As shown in FIG. 6D, the electrode portion 46 may be divided into at least one of the electrode portions formed on the inner and outer surfaces, and the ultrasonic transducers 42 and 52 may be divided and arranged. The same effect can be obtained. The number of divisions of the electrodes is arbitrary, It need not be symmetric.

(Fifth embodiment)

An ultrasonic transducer as an example of the ultrasonic sensor according to the fifth embodiment of the present invention will be described with reference to FIG. FIG. 7 is a perspective view of the appearance of an ultrasonic transducer 61 according to the fifth embodiment, and FIG. 7 is a cross-sectional view for explaining the internal structure of a front surface A in FIG. In fact, it is covered on the side of the housing. In addition, the same reference numerals are given to members common to the fifth embodiment and the above-described first to fourth embodiments. The propagation medium 6F corresponds to the propagation medium 6 or 6A of the first embodiment, and the housing 9F corresponds to the housing 9 or 9A of the first embodiment.

Hereinafter, features of the ultrasonic transducer 61 according to the fifth embodiment will be described. The ultrasonic transducer 1 according to the first embodiment, the ultrasonic transducer 11 according to the second embodiment 11 , 21, the ultrasonic transducer 31 of the third embodiment, and the same parts and corresponding parts as those of the ultrasonic transducers 41, 51 of the fourth embodiment are not described. . The ultrasonic transducer 61 of the fifth embodiment has a rectangular or conical part in the ultrasonic transducers 41, 51 of the fourth embodiment, and has a rectangular shape. A rectangular plate-shaped terminal plate 69 X is fixed to the lower end of the plate-shaped side portion 69 g, and a triangular prism-shaped reflector 64 is fixed around the side portion 69 g and the terminal plate 69 X. A rectangular plate-like upper plate 69 m is fixed to the upper end of the rectangular plate-like center axis 69 k so as to protrude like a flange and is symmetrical with respect to the center line C. Each of the ultrasonic transducers 6 2 and each of the acoustic matching layers 63 are rectangular plates and fixed to the inner surface of the central axis 69 k, and each of the acoustic matching layers 6 is provided outside the ultrasonic transducer 62. 3 are located. Each of the propagation medium portions 6F has a first surface region 7 parallel to the vibration surface of each of the ultrasonic transducers 62 and a second surface region 8 in contact with a fluid that fills the surrounding space. It is in contact with the reflector 64 provided adjacent to 6F at the third surface region 65. The reflector 64 has the same material and the same inclination angle as the reflector 44.

The difference between the fifth embodiment and the fourth embodiment is that the transmission and reception of ultrasonic waves in the ultrasonic transducer 61 of the fifth embodiment are symmetrical with respect to the center line C in the left and right directions in FIG. Also in this case, the ultrasonic waves pass through the acoustic matching layer 63, respectively. The ultrasonic wave that is radiated to the propagation medium portion 6F under the condition of approximately 1 in efficiency and propagated in the propagation medium portion 6F is reflected at the third surface region 65, which is the interface with the reflector 64, with approximately 1 efficiency. Then, the direction is changed to the second surface region 8 side. Further, the ultrasonic wave is refracted at the second surface region 8 which is the interface between the propagation medium portion 6F and the fluid filling the surrounding space, and is radiated to the fluid filling the surrounding space in a state of almost efficiency 1. In addition, regarding the ultrasonic wave propagating from the transmission direction, a path opposite to that in the case of the transmission is established, and the ultrasonic wave incident on the ultrasonic transducer 61 into the second surface area 8 with almost the efficiency 1 is Then, the light propagates through the propagation medium portion 6F, is reflected by the third surface region 65, which is the interface with the reflector 64, with almost the condition of efficiency 1, and reaches the ultrasonic vibrator 62. It is converted into an electric signal in 2.

With the above configuration, the ultrasonic transducer 61 can transmit and receive the ultrasonic waves with high efficiency to the fluid that fills the surrounding space, and can provide the same effects as the first embodiment. In addition, the ultrasonic transducer 61 has a structure capable of transmitting and receiving waves in the left and right directions. When the surrounding space is gas, the transmitting and receiving waves are almost horizontal, and the left and right objects are detected. Application becomes possible.

(Sixth embodiment)

An ultrasonic transducer as an example of the ultrasonic sensor according to the sixth embodiment of the present invention will be described with reference to FIGS. 8A and 8B. 8A and 8B are perspective views of a case where a plurality of ultrasonic transducers 71-1, 71-2, 71-3, 71-4 in the sixth embodiment are arranged. The same reference numerals are given to members common to the sixth embodiment and the above-described first to fifth embodiments. The propagation medium portion 6G corresponds to the propagation medium portion 6 of the first embodiment or the propagation medium portion 6F of the fifth embodiment, and the housing 9G is the housing 9 or the fifth embodiment of the first embodiment. The center axis 79 k corresponds to the center axis 69 k of the fifth embodiment, the side part 79 g corresponds to the side part 69 g of the fifth embodiment, The terminal plate 79X corresponds to the terminal plate _69X of the fifth embodiment, the reflector 74 corresponds to the reflector 64 of the fifth embodiment, and the upper plate 79m corresponds to the upper portion of the fifth embodiment. It corresponds to a plate 69 m.

Hereinafter, features of the ultrasonic transducers 7 1-1, 7 1-2, 7 1-3, 7 1-4 of the sixth embodiment will be described, and the same parts as in the other embodiments and The description of the corresponding parts is omitted. Each of the ultrasonic transducers 71-1, 71-2, 71-3, 71-4 of the sixth embodiment is obtained by dividing the ultrasonic transducer 61 of the fifth embodiment on a center line C. It is made. Therefore, transmission and reception of ultrasonic waves are limited to only one direction, but transmission and reception of ultrasonic waves are performed with high efficiency as in the fifth embodiment, and the same effects as in the first embodiment can be obtained. . When the surrounding space is a gas, the transmitted and received waves are almost horizontal, which makes it possible to apply it to object sensing and the like.

Figure 8A shows a configuration in which four ultrasonic transducers 71-1, 71-2, 71-3, and 71-4 can be used to transmit and receive ultrasonic waves in front, back, left, and right. In this configuration, three transducers 71-1, 71-2, and 71-3 can be used to transmit and receive in three directions at 120-degree intervals. As shown in Fig. 8A and Fig. 8B, by arranging a plurality of ultrasonic transducers 71 in any number and in any direction, it is possible to control the directivity corresponding to the application and expand the application range. Can be.

(Seventh embodiment)

With reference to FIGS. 9A, 9B, and 9C, an application device of an ultrasonic transducer as an example of the ultrasonic sensor according to the seventh embodiment of the present invention will be described. Figure 9A shows an obstacle detection system for a self-propelled robot such as a cleaning robot, Figure 9B shows an obstacle detection system around a car, and Figure 9C shows the case of application to an ultrasonic flowmeter. . 9A, 9B, and 9C, 81, 81A, 81B, 81C, 81D, and 81E show the seventh embodiment of the present invention, in particular, the first embodiment, the second embodiment, An ultrasonic transducer capable of transmitting and receiving ultrasonic waves in a substantially horizontal direction shown in any of the fourth embodiment, the fifth embodiment and the sixth embodiment is shown. 82, 82 A, 82 B, 82 C, 82 D, and 82 E are the directional characteristic areas of the ultrasonic waves transmitted and received by the ultrasonic transducers 81, 81 A, 81 B, 81 C, 8 ID, 81 E, and 83 A self-propelled robot, 84A, 84B, 84C, 84D, 84E is an obstacle, 85 is a car, and 86 is a measurement channel.

In FIG. 9A, in the ultrasonic transducer 81A, the surface of the housing and the second surface region 8 are arranged substantially flush with each other near the top of the housing of the self-propelled robot 83. . According to the ultrasonic transducer 81A of the seventh embodiment of the present invention, as shown in FIG. 9A, the directional characteristic area 82A of the ultrasonic wave is substantially horizontal (parallel) with the floor surface 88A. thing And scanning in the circumferential direction is possible. Therefore, there is no need to disperse the ultrasonic transducer 81 A around the housing, and to provide a special mechanism in the housing to direct the ultrasonic transducer 81 A to the periphery. Without this, it is possible to detect obstacles in all directions of the self-propelled robot 83.

In FIG. 9B, the ultrasonic transducers 8 ID, 81 E, 81 B, and 81 C are

The bottom surface of the bumper section at the front and rear ends of the body and the wall near the front and rear ends of the roof of the body are almost flush with each other without special projections. Similarly to FIG. 9A, the directional characteristic regions 82 D, 82 E, 82 B, and 82 C of the transmitted and received ultrasonic waves can be made substantially horizontal (parallel) to the ground surface 88 B. Therefore, as shown in Fig. 9B, obstacles 84 D, 84 E on the ground existing in the blind spot before and after the car 85, and obstacles 84 4B, 84 C can be detected, and it can be realized without providing a projection for the ultrasonic transducer especially on the roof, so that the degree of freedom in design and the like is not impaired.

In FIG. 9C, the ultrasonic transducer 81 is arranged flush with the inner wall surface of the measurement flow channel 86. The directional area 82 of the transmitted / received ultrasonic wave is substantially parallel to the flow path, and the ultrasonic wave is transmitted / received between the ultrasonic wave transmitter / receiver 81 facing the ultrasonic wave transmitter / receiver 81. In this case, there is no need to face the ultrasonic transducer 81 directly, so there is no need to provide concave or convex parts in the normal flow path, and the state of fluid movement in the flow path is constantly maintained. Highly accurate flow rate measurement is possible. This will be described in detail below as an eighth embodiment. A transmitting circuit 70 1 for driving the ultrasonic vibrator 81, a receiving circuit 70 2 for amplifying the ultrasonic wave received by the other ultrasonic vibrator 81, and performing band limiting, etc. Switching circuit 703 for changing the direction of the signal, a time measuring section 704 for measuring the propagation time based on the output from the receiving circuit 702, and an output value from the time measuring section 704. The flow rate calculation unit 705 for obtaining the flow rate based on the flow rate, the display unit 706 for displaying the flow rate calculated by the flow rate calculation unit 705, and the control unit 707 for controlling the measurement timing and the like Have. Therefore, an ultrasonic wave is transmitted from one ultrasonic oscillator 81 to the other ultrasonic oscillator 81, and the ultrasonic wave that has passed through the fluid to be measured, such as gas, is transmitted to the other ultrasonic oscillator 81. Upon reception, the time measuring unit 704 measures the propagation time between the ultrasonic transducers 81 and 81. Then, conversely, the other ultrasonic transducer 8 The ultrasonic wave is transmitted from 1 to the above-mentioned one ultrasonic vibrator 81, and the ultrasonic wave passing through the fluid to be measured such as gas is received by the one ultrasonic vibrator 81, thereby measuring time. The section 704 measures the propagation time between the ultrasonic transducers 81 and 81. As described above, the propagation time of the ultrasonic wave is measured between the pair of ultrasonic transducers 81 and 81 a predetermined number of times, and the flow rate calculation unit 705 uses the measured value to measure the fluid to be measured such as gas. Is calculated by the flow rate calculation unit 705. Therefore, each of the ultrasonic transducers 81 and 81 can transmit and receive. Here, the transmission circuit 701 to the control unit 707 constitute a flow rate calculation system.

(Eighth embodiment)

With reference to FIGS. 12A to 17, the flow rate of a fluid is determined by ultrasonic waves, which is an example of an applied device of an ultrasonic transducer as an example of the ultrasonic sensor according to the eighth embodiment of the present invention. The ultrasonic flowmeter to be measured will be described.

First, before describing the ultrasonic flowmeter of the eighth embodiment, a conventional ultrasonic flowmeter will be described.

In recent years, an ultrasonic flowmeter that measures the moving speed of a fluid by measuring the time that ultrasonic waves travel through a predetermined propagation path and measures the flow rate from the measured value is used for controlling gas meters and chemical reactions. It is being used.

Hereinafter, the measurement principle of the conventional ultrasonic flowmeter will be described with reference to FIG. In the ultrasonic flowmeter shown in FIG. 17, the fluid in the pipe flows at the speed V in the direction indicated by the arrow V in FIG. A pair of ultrasonic transducers 401 and 402 are installed facing each other on the tube wall 403 of the ultrasonic flowmeter. Each of the ultrasonic transducers 401 and 402 is provided with a conversion element (transducer) that converts electric energy into mechanical energy and converts mechanical energy into electric energy. This conversion element is composed of, for example, a piezoelectric vibrator such as a piezoelectric ceramic, and exhibits resonance characteristics like a piezoelectric buzzer or a piezoelectric oscillator.

First, the operation of the ultrasonic flowmeter will be described for a case where the ultrasonic transducer 401 is used as an ultrasonic transducer and the ultrasonic transducer 402 is used as an ultrasonic transducer. .

A supersonic wave with an AC voltage having a frequency near the resonance frequency of the ultrasonic transducer 401 When applied to the piezoelectric vibrator of the wave transmitter / receiver 401, the ultrasonic transmitter / receiver 401 emits an ultrasonic wave into a fluid in the pipe. This ultrasonic wave propagates along the propagation path L1 and reaches the ultrasonic transducer 402. The piezoelectric vibrator of the ultrasonic transducer 402 receives this ultrasonic wave and outputs a voltage signal.

Thereafter, the ultrasonic transducer 402 is operated as an ultrasonic transducer. Specifically, by applying an AC voltage having a frequency near the resonance frequency of the ultrasonic transducer 402 to the piezoelectric vibrator of the ultrasonic transducer 402, the ultrasonic transducer 402 Emits ultrasonic waves into the fluid in the tube. The ultrasonic wave propagates along the propagation path L2 and reaches the ultrasonic transducer 401. The piezoelectric vibrator of the ultrasonic transducer 401 receives this ultrasonic wave and outputs a voltage signal.

As described above, the ultrasonic transducers 401 and 402 can each function as a receiver and a transmitter as a single ultrasonic transducer. . In this ultrasonic flow meter, if an AC voltage is applied continuously, ultrasonic waves are continuously emitted from the ultrasonic transducer, making it difficult to measure the propagation time. Is used as a drive voltage.

When a driving burst voltage signal is applied to the ultrasonic transducer 410 and an ultrasonic burst signal is emitted from the ultrasonic transducer 410, the ultrasonic burst signal has a propagation path L 1 having a distance L. And arrives at the ultrasonic transducer 402 after time t.

The ultrasonic transducer 402 can convert only the transmitted ultrasonic burst signal into an electric burst signal with a high S / N ratio. With the electric burst signal as a trigger, a driving burst voltage signal is applied again to the ultrasonic transducer 401 to emit an ultrasonic burst signal.

Such a device is called a "singing-around device". Also, the time required for an ultrasonic pulse to reach the ultrasonic transducer 410 from the ultrasonic transducer 401 is called "sing-around period", and the reciprocal thereof is called "sing.around frequency". .

In the ultrasonic flow meter shown in Fig. 17, the flow velocity of the fluid flowing through the tube is V, the velocity of the ultrasonic wave in the fluid is C, and the angle between the direction in which the fluid flows and the propagation direction of the ultrasonic pulse is 0. Further, the ultrasonic transducer 410 is used as a transmitter, and the ultrasonic transducer 402 is used as a receiver. In this case, the time (singing-around period) during which the ultrasonic pulse emitted from the ultrasonic transducer 401 arrives at the ultrasonic transducer 402 is defined as sing ■ around frequency f. At this time, the following equation (4) holds.

f! == 1 / t, = (C + V cos Θ) / L (4) Conversely, ultrasonic transducer 402 was used as the transmitter, and ultrasonic transducer 401 was used as the receiver. If the sing-around period is t ₂ and the sing-around frequency f ₂ , the following equation (5) holds.

f ₂ = 1 / t ₂ = (CV cos 0) / L · · · (5) Based on the above formulas (4) and (5), the frequency difference Δf between both singing-around frequencies is expressed by the following formula ( 6).

F = ί 丄 1 f ₂ = 2Vc os 0 / L ■ ■ · As can be seen from equation (6), the flow velocity V of the fluid is obtained from the distance L of the ultrasonic wave propagation path and the frequency difference Λ f be able to. Then, the flow rate can be determined from the flow velocity V.

In the ultrasonic flow meter of FIG. 17, a matching layer (not shown) is provided on the ultrasonic wave transmitting / receiving surface of the piezoelectric vibrator of the ultrasonic wave transmitter / receiver. This is because the difference in intrinsic acoustic impedance (hereinafter referred to as “acoustic impedance”) between the fluid to be measured and the piezoelectric element is reduced by a layer having an intermediate acoustic impedance (matching layer). This is to suppress the reflection of ultrasonic waves at the interface between media having different acoustic impedances. If there is an interface with a large difference in acoustic impedance in the propagation path of the ultrasonic wave, there is a disadvantage that the ultrasonic wave emitted from the ultrasonic transducer does not sufficiently enter the fluid to be measured, and the flow rate is measured. Measurement becomes impossible, or the measurement accuracy is greatly reduced. Therefore, it is important to properly set the acoustic impedance of the matching layer in order to avoid such inconveniences and improve the measurement accuracy of the ultrasonic flowmeter. The acoustic impedance is generally defined by the following equation (7). Acoustic impedance = (density) X (sound velocity) · · · ■ (7) The acoustic impedance of a piezoelectric vibrator that generates ultrasonic vibration is, for example, about 30 x 10 ⁶ kg · m- ² · s- Has an acoustic impedance of about 400 kg-m— ² · s- ¹ ). When measuring the air velocity, the acoustic input of the matching layer Impedance is ^{0. 1 1 X 1 0 6} kg · m- 2 · s- one extent to the set it is preferred arbitrariness.

Conventionally, in order to form a matching layer having an acoustic impedance intermediate between the piezoelectric vibrator and air, a material obtained by solidifying a relatively low-density material (for example, glass vanolane or plastic vanolane) with resin is used. It is used.

However, even when the above-described matching layer is used, when ultrasonic waves are propagated from a piezoelectric vibrator into a gas such as air, there is a problem that a transmission loss is inevitably generated and measurement sensitivity is reduced. . The reason that it is difficult to efficiently transmit ultrasonic waves from a solid to a gas is that the acoustic impedance of the gas is much smaller than that of the solid, and even if a matching layer is interposed, the ultrasonic waves are strong at the interface. This is because reflection occurs.

Also, in the ultrasonic flowmeter of the type shown in Fig. 17, a cavity for arranging the ultrasonic transducer is required inside the flow path of the flow measurement unit. May cause turbulence in body flow. Also, for trace chemical analysis, the flow rate itself becomes extremely small, so it is necessary to miniaturize the flow path. In such a case, the conventional configuration has a problem that the ultrasonic transducer cannot be arranged in the flow path, and therefore cannot be applied to the measurement of a very small flow rate.

The eighth embodiment of the present invention has been made in view of the above-described problem, and its purpose is to measure a very small amount of flow without disturbing the flow inside the flow path which is a flow measurement unit. It is an object of the present invention to provide a high-sensitivity ultrasonic flowmeter capable of performing the method.

An ultrasonic flowmeter according to an eighth embodiment of the present invention includes a flow measurement unit having an inner wall that defines a flow path of a fluid to be measured, and an ultrasonic flowmeter provided outside a flow path space surrounded by the inner wall of the flow measurement unit. At least one ultrasonic transducer for transmitting and / or receiving or transmitting ultrasonic waves, and a propagation medium disposed between the ultrasonic transducer and the flow path space and forming a propagation path of the ultrasonic waves. An ultrasonic flowmeter comprising: a density P of the propagation medium part; a sound velocity C in the propagation medium part; a density p _{2 of} the fluid to be measured; and a sound velocity C _{2 in the} fluid to be measured, p ₂ / _{P l} ) <{C _x / C ₂ ) <1 In a preferred embodiment, the number of the ultrasonic vibrators is plural, and the first ultrasonic vibrator among the plural ultrasonic vibrators is a second ultrasonic vibrator among the plural ultrasonic vibrators. The second ultrasonic vibrator is arranged to emit ultrasonic waves to the ultrasonic vibrator, and the second ultrasonic vibrator is arranged to emit ultrasonic waves to the first ultrasonic vibrator.

In a preferred embodiment, the propagation medium portion has a first surface region facing the ultrasonic vibration surface of the ultrasonic transducer, and a second surface region facing the flow path space. The second surface region of the propagation medium section is inclined with respect to the first surface region.

In a preferred embodiment, the first surface region of the propagation medium portion is inclined with respect to the flow direction of the fluid to be measured in the flow channel space, and the second surface region is formed in the flow channel space. It is parallel to the flow direction of the fluid to be measured.

In a preferred embodiment, the second surface region of the propagation medium section does not substantially form a step with the inner wall of the flow rate measurement section.

In a preferred embodiment, the density P of the propagation medium portion is an incident angle of an ultrasonic wave to an interface between the propagation medium portion and the fluid to be measured, and the density p _{2 of} the fluid to be measured is from the interface. The angle of incidence of the ultrasonic wave 0 ₂ into the fluid to be measured is

The structure is such that the relationship of p-cote ₂ / cote is almost satisfied.

In a preferred embodiment, the fluid to be measured, the density P ₂ is 1 0 kg · m one ³ hereinafter gases.

In a preferred embodiment, the propagation medium portion is formed from a dried gel of an inorganic acid or an organic polymer.

In a preferred embodiment, the solid skeleton of the dried gel is hydrophobically ridden. In a preferred embodiment, the density of the dried gel is 500 _{kg //} m ³ or less, and the average pore diameter of the dried gel is 100 nm or less.

In a preferred embodiment, a matching layer is provided between the ultrasonic vibrator and the propagation medium part, and acoustically matches the ultrasonic vibrator and the propagation medium part.

In a preferred embodiment, the measurement is performed in a direction perpendicular to the flow velocity direction of the fluid to be measured. The size of the flow path space in the flow velocity measuring section is 1 Z 2 or less of the wavelength in the fluid to be measured at the center frequency of the ultrasonic wave.

In a preferred embodiment, the ultrasonic transducer is configured to form a convergent sound field.

In a preferred embodiment, the first surface region of the propagation medium section is curved so as to form a lens surface.

An ultrasonic flowmeter according to the present invention is provided with a flow measurement unit having an inner wall that defines a gas flow path, and provided outside a flow path space surrounded by an inner wall of the flow measurement unit, and transmits and / or transmits ultrasonic waves. A pair of ultrasonic transducers for receiving, and a pair of propagation medium units disposed between each of the pair of ultrasonic transducers and the flow path space, and refracting a propagation path of the ultrasonic wave, The propagation medium portion has a first surface region facing the ultrasonic vibration surface of the ultrasonic transducer, and a second surface region facing the flow path space. The one surface region is inclined with respect to the flow direction of the gas in the flow channel space, and the second surface region is substantially parallel to the flow direction of the gas in the flow channel space.

In the ultrasonic transducer according to the eighth embodiment of the present invention, the surface (first surface region) inclined with respect to the flow direction of the fluid to be measured and the surface substantially parallel to the flow direction of the fluid to be measured

(Second surface region) is disposed between the ultrasonic transducer and the fluid to be measured. The second surface region of the propagation medium portion is preferably aligned with a surface defining a fluid flow path so as not to disturb the flow of the fluid.

Hereinafter, an eighth embodiment of the present invention will be described with reference to the drawings.

First, an ultrasonic flowmeter according to an eighth embodiment of the present invention will be described with reference to FIGS. 12A and 12B. FIG. 12A shows a cross section along the longitudinal direction of the ultrasonic flowmeter 310 in the eighth embodiment, and FIG. 12B shows the longitudinal direction of the ultrasonic flowmeter 310 and FIG. A cross section orthogonal to the line B—B of FIG. The illustrated ultrasonic flow meter 310 includes a tubular flow measuring section 304 having an inner wall 330 that defines a flow path of a fluid to be measured, and an outer flow path space 309 surrounded by an inner wall 340 of the flow measuring section 304. And a pair of ultrasonic transducers (ultrasonic transducers) 301 1a and 301b for transmitting and / or receiving ultrasonic waves, and ultrasonic transducers 301a and 301b Propagation medium portions 303a and 303b are disposed between the space 309 and form a propagation path of ultrasonic waves. It is assumed that the fluid to be measured flows in the direction of the arrow 305 inside the flow path space 309 surrounded by the inner wall 340 of the flow rate measuring section 304. The ultrasonic transducers (ultrasonic transducers) 301a and 301b are the ultrasonic transducers of any of the first to sixth embodiments. The propagation medium parts 303a and 303b are the propagation medium parts 6, 6A, 6B, 6C, 6D, 6E,

Corresponds to 6 F, 6 G. The casing is not shown for simplicity.

In the eighth embodiment, the ultrasonic wave emitting surface of the ultrasonic transducer 301a is inclined with respect to the flow direction 305 of the fluid to be measured, and the ultrasonic wave emitted from the ultrasonic transducer 301a is The light obliquely enters the inner wall of the flow measurement unit 304. Then, the ultrasonic wave is refracted at the interface between the transmission medium part 303a and the fluid to be measured, passes through the propagation path 306, and is received by one ultrasonic transducer 301b.

A cross section (a cross section perpendicular to the flow direction 305) of the channel space 309 in the eighth embodiment is rectangular as shown in FIG. 12B. The flow rate measuring section 304 of the eighth embodiment is manufactured by fixing parts 304a and 304b with a sealing material 304c. The shape of the channel space 306 is not limited to the illustrated one, but may be another shape (for example, circular).

The propagation medium portions 303a and 303b are composed of a first surface region 331, which faces the ultrasonic vibration surface of the ultrasonic transducers 30La and 301b, and a second surface, which faces the flow path space 309. Region 332. In the eighth embodiment, the density of the propagation medium portions 303 a and 303 b is p ₁ , the sound speed of the propagation medium portions 303 a and 303 b is C, the density of the fluid to be measured is P ₂ , and the density of the fluid to be measured is P ₂ . When the sound velocity is C ₂ , the materials of the propagation medium portions 303 a and 303 b are selected so that the relationship shown in the following equation (8) is satisfied.

(P ₂ / P ₁ ) <(C C ₂ ) <1 (8) When measuring the gas flow rate, it is difficult to find a material that satisfies the above conditions. The reason for this is that there is less solid material with a smaller sound velocity than the sound velocity C _{2 of} gas. In the eighth embodiment, in order to realize the propagation medium portions 303 a and 303 b satisfying the above conditions, the propagation medium portions 303 a and 303 b are formed from a dried gel of an inorganic oxide or an organic polymer. Has formed. The solid skeleton of the dried gel used in the eighth embodiment is hydrophobized, and its density is 500 kg / m ³ or less. This dry gel is a nanoporous dry gel having an average pore diameter of 100 nm or less (nanoporous dry gel).

The solid skeleton of the dried gel of the inorganic oxide preferably contains at least silicon oxide (silicone) or aluminum oxide (alumina). The solid skeleton of the dried gel of the organic polymer can be made of a general thermosetting resin or thermoplastic resin. For example, polyurethane, polyurea, phenol-cured resin, polyacrylamide, polymethyl methacrylate, or the like can be used.

The propagation medium portion 3 0 3 a, 3 0 3 b, for example, in the case of forming a nanoporous Drying gel consisting mainly of silica force, if the density p is 20 0 kg / m ^3, the sound velocity 1 It can be set in the range from about 00 s to about 180 m / s. If the fluid to be measured is air, the density p ₂ of air is 1.22 kg / m ³ and the sound velocity C ₂ is 340 m / s, so the above propagation medium sections 303 a and 303 b are adopted. Thus, the relationship between p 2/0 and C Cs is satisfied at the same time, and (P SZP

_X / C ₂ ) can be satisfied. When measuring the gas flow rate of natural gas, etc., the propagation medium sections 303 a and 303 b have a density p of 100 to 300 kg / m ³ and a sound velocity of 100 to 30 OmZs. Is preferred.

Each of the ultrasonic transducers 301a and 301b has a piezoelectric body functioning as an ultrasonic vibrator, and can transmit, transmit, or receive ultrasonic waves. As the piezoelectric body, a piezoelectric ceramic is preferably used.

In the ultrasonic flow measuring device 310 of the eighth embodiment, the matching layer 302 a is provided between the propagation medium portion 303 a and the ultrasonic transducer 30 la, and the propagation medium portion A matching layer 302b is provided between 303b and the ultrasonic transducer 301b. Matching layer 30 2 a, 3 0 2 b is an ultrasonic transducer 3 0 1 a, 3 0 1 b of the pressure conductive ceramic is an ultrasonic source (acoustic ^{impedance: 3 0 X 1 0 6 kg} 'm- 2 ■ s —) And a function to enhance acoustic matching between the transmission medium sections 303 a and 303 b.

When forming a nanoporous dry gel (acoustic impedance ^{3 X 1 0 4 kg · m-} 2 · s- 1 ]) propagation medium portion 3 0 3 a, 3 0 3 b mainly composed of silica, acoustic I impedance is 1 X 1 0 ⁶ kg ■ m one ² - ^s-1) by employing a material matching layer 3 0 2 produced from a, 3 0 2 b nearby, the propagation efficiency of the ultrasonic energy approximately 1, Specifically, it can be 0.95 or more. Such a material can be realized by a composite material obtained by solidifying hollow glass spheres with a resin material. It is preferable that the thickness of the matching layers 302a and 302b be set to 1/4 wavelength of the ultrasonic wave to be used.

Next, the manner in which ultrasonic waves propagate from the propagation medium portion 303a into the fluid to be measured will be described in detail with reference to FIG.

From the above-described arrangement relationship, the ultrasonic wave enters the interface S along a direction inclined from the normal direction of the interface S between the propagation medium portion 303 a and the fluid to be measured. Let Θ be the angle of incidence of the ultrasonic wave with respect to the normal direction to the interface (0 ° <θ <90 °). At this time, the ultrasonic wave is refracted at the interface S between the propagation medium part 303 a and the fluid to be measured, and enters the fluid to be measured at an angle (entrance angle) Θ ₂ with respect to the normal direction of the interface S. Naru (es ^.

In the above eighth embodiment, when p _{2 of the} fluid to be measured is given, various parameters (p （and θ ₂ ) are set so as to substantially satisfy the relationship of the following equation (9). .

(ρ ₂ / β _r = (cot Θ ₂ Zc ot Θ J) With such a setting, the propagation efficiency of the ultrasonic energy from the propagation medium portion 303 a to the fluid to be measured becomes almost 1. At this time, the incident angle 6 satisfies the condition expressed by the following equation (10).

(cot) ²

= [(C Bruno _{^{c 2) 2 - 1] /}} [2 2 - (c 2) 2]

(10) Therefore, C of the propagation medium portion 303 and p of the fluid to be measured. , C ₂ is Sadama Then, the angle of incidence 0 is determined by equation (10). If the incident angle 0 is determined, the approach angle θ ₂ is determined by equation (9).

Once the angle of incidence θ and the angle of approach θ ₂ are determined, the inclination angle of the first surface area 3 31 of the propagation medium section 303 a and the interval between the two ultrasonic transducers 310 a and 310 b, etc. Also decide.

The above applies to ultrasonic waves as they are received.

In the eighth embodiment, the propagation speeds C i of the propagation medium portions 303 a and 303 b are set to 180 / s by forming the propagation medium portions 303 a and 303 b from the aforementioned materials. , it is possible to set the density p to 2 00 k gZm ^3. When measuring the flow rate of air, the density p ₂ of the fluid to be measured (air) is 1.22 kg / sonic velocity C ₂ is 340 s, so from the relations of equations (9) and (10), The incident angle Θ i may be set to 32 °, and the approach angle 0 ₂ may be set to 89 °. Since the approach angle θ ₂ is close to 90 °, the ultrasonic wave in the fluid to be measured propagates in a direction substantially parallel to the flow direction 304.

The size H (see FIG. 12A) of the flow path space 309 surrounded by the inner wall 340 of the flow rate measuring section 304 in the eighth embodiment is ideally less than 1/2 wavelength of the ultrasonic wave in the fluid to be measured. Is preferably set to 1/4 wavelength or less. By setting the size of the channel space 309 to such a size, the appearance of a propagation mode due to sound wave reflection in the channel space 309 can be suppressed, and the accuracy of time measurement can be improved. For example, when the wavelength of the ultrasonic wave to be used; L is about 4 mm, the size H of the channel space 309 can be set to about 2 mm. In this case, assuming that the minimum flow velocity of the object to be measured is 1 mm / s and the measurement system of the propagation time is Ins (nanosecond), the horizontal direction of the ultrasonic transducers 301a and 301b is assumed. The spacing can be set around 120 mm.

According to the eighth embodiment, since propagation loss hardly occurs at the interface S between the propagation medium portion 303 a 303 b and the fluid to be measured, it is necessary to match both acoustic impedances at the interface S. There is no.

Note that the propagation medium portions 303 a and 303 b need not be made of a material having a uniform density pi and a sound speed Ci throughout the entire material, but a plurality of materials having different densities pi and sound speeds Ci. It may have a stacked structure in which layers are stacked. With such a laminated structure, the ultrasonic wave may not travel straight through the propagation medium sections 303a and 303b. Some power No problem. The important point is that in the region near the interface between the propagation medium sections 303a and 303b and the fluid to be measured, the density of the propagation medium sections 303a and 303b so as to satisfy the above equation pi and sound velocity C and the angle of incidence Θi are set.

Further, as shown in FIG. 12A, the ultrasonic flow measuring device 310 is provided with a transmitting circuit 70 1 for driving the ultrasonic vibrator 81 and a receiving circuit 71 1 for receiving the other ultrasonic vibrator 81. The propagation time is measured based on the output from the receiving circuit 702 for amplifying the transmitted ultrasonic wave, band limitation, etc., the switching circuit 703 for changing the direction of transmission and reception, and the receiving circuit 702. Time measurement section 704, flow rate calculation section 705 for calculating flow rate based on the output value from time measurement section 704, table for displaying flow rate calculated by flow rate calculation section 705 An indicator 706 and a controller 707 for controlling measurement timing and the like are provided. Therefore, ultrasonic waves are transmitted from one ultrasonic transducer 301a or 301b to the other ultrasonic transducer 301b or 301a, and the fluid to be measured such as gas is transmitted. The transmitted ultrasonic wave is received by the other ultrasonic transducer 301b, and the time measuring unit 704 measures the propagation time between the ultrasonic transducers 301a or 301b. I do. Next, conversely, on the contrary, the ultrasonic wave is transmitted from the other ultrasonic vibrator 301 b to the one ultrasonic vibrator 301 a, and the ultrasonic wave that has passed through the fluid to be measured such as gas is The time measurement unit 704 measures the propagation time between the ultrasonic transducers 301a and 301b by being received by one of the ultrasonic transducers 301a or 301b. . As described above, the propagation time of the ultrasonic wave is measured between the pair of ultrasonic transducers 301a and 301b a predetermined number of times, and the flow rate calculation unit 705 uses the value to calculate the gas or the like based on the value. The flow rate of the fluid to be measured is calculated by the flow rate calculation unit 705. Therefore, each of the ultrasonic transducers 301a and 310b can transmit and receive. Here, the transmission circuit 701 to the control unit 707 constitute a flow rate calculation system.

Next, the operation of the ultrasonic flowmeter according to the eighth embodiment will be described.

First, the transmission circuit 701, which also serves as the drive circuit in FIG. 12B, has a frequency near the resonance frequency (for example, about 100 kHz to 1 MHz) to the ultrasonic transmitter 3 O la. AC voltage is applied. As a result, the ultrasonic transducer 301a emits an ultrasonic wave to the propagation medium portion 303a through the matching layer 302a under the condition of approximately 1 efficiency.

The sound wave that has propagated through the propagation medium section 303 a and the propagation medium section 303 a It is refracted at the interface with, radiated into the channel space 309 at a state of almost efficiency 1, and propagates inside the fluid to be measured. Thereafter, the ultrasonic waves reach the ultrasonic transducer 30 Olb through the propagation medium portion 303 b and the matching layer 302 b provided on the opposite side. The ultrasonic transducer 301b converts the received ultrasonic waves into a voltage, and generates a voltage signal (electric signal). The method of measuring the propagation time of the ultrasonic wave based on the electric signal by the flow rate calculation unit 705 and converting the flow rate into the flow rate is the same as that of the conventional technique. Examples of the configuration of the drive circuit are described in JP-A-2000-29045 and JP-A-2000-29047.

According to the eighth embodiment, the propagation medium portions 303a and 303b exhibiting appropriate densities p and sound speeds are provided, and the ultrasonic waves are refracted at an appropriate angle. The flow loss can be reduced to almost zero, and the flow rate can be measured with a good S / N ratio. Then, according to the eighth embodiment, it is possible to easily measure the flow rate of a gas (for example, hydrogen gas or the like), which was extremely difficult to measure with a conventional ultrasonic flowmeter.

Furthermore, according to the eighth embodiment, there is no large unevenness or step that disturbs the flow inside the flow path space 309 of the flow rate measuring section 304, and extremely stable flow rate measurement can be performed. Further, since the ultrasonic transducer is arranged outside the flow path space 309, the size of the flow path space 309 can be arbitrarily designed regardless of the size of the ultrasonic transducer. As a result, it becomes possible to reduce the size of the flow path space 309 and measure a very small amount of flow.

(Ninth embodiment)

An ultrasonic flowmeter as an example of an ultrasonic sensor according to the ninth embodiment of the present invention will be described with reference to FIG. FIG. 14 shows a cross section along the longitudinal direction of the ultrasonic flowmeter 320 in the ninth embodiment. The same reference numerals are given to members common to the ninth embodiment and the above-described eighth embodiment. Hereinafter, features of the ultrasonic flowmeter 320 of the ninth embodiment will be described, and description of the same parts as the ultrasonic flowmeter 310 of the eighth embodiment will be omitted. In the ultrasonic flowmeter 320 of the ninth embodiment, the ultrasonic transducers 301a and 301b are configured to form a convergent sound field. Specifically, the propagation medium section 3 0 8 The first surface area of a, 308b is curved to form a lens surface. Accordingly, the surface of the matching layer 308 on the side of the fluid to be measured is concave. With such a configuration, the ultrasonic waves transmitted from the ultrasonic transducer 3Ola converge in the propagation medium 308a. Due to this convergence effect, it is possible to transmit and receive ultrasonic waves at a higher sound pressure by using an ultrasonic oscillator having the same performance, so that the SZN ratio can be further improved.

In the eighth and ninth embodiments described above, in any case, the first surface region 331 of the propagation medium portion is inclined with respect to the flow velocity direction 305 of the fluid to be measured in the channel space 309, and the second surface region Although 332 is parallel to the flow direction 305 of the fluid to be measured in the channel space 309, the present invention is not limited to such a configuration. For example, as shown in FIG. 15A, a configuration is adopted in which the second surface area 332 of the propagation medium sections 303a and 303b is inclined with respect to the flow direction 305 of the fluid to be measured in the flow path space 309. Is also good. According to such a configuration, the interval between the two ultrasonic transducers can be reduced. However, in the configuration of FIG. 15A, a step is formed between the inner wall 340 of the flow rate measuring unit 304 and the second surface region 332 of the propagation medium units 303a and 303b. In order to reduce or eliminate this step, for example, as shown in FIGS. 15B and 15C, an inclined surface is formed on a part of the inner wall 340 of the flow rate measuring unit 304, and the inclined surface is formed in the propagation medium parts 303a and 303. What is necessary is just to match with the 2nd surface area 332 of b.

It is preferable that the second surface region 332 of the propagation medium sections 303a and 303b does not substantially form a step with the inner wall 340 of the flow rate measurement section 304, but flow turbulence does not become a major problem. In this case, steps or irregularities as shown in FIGS. 16A and 16B may exist.

In any of the above eighth and ninth embodiments, the configuration of the pair of ultrasonic transducers is substantially the same, and a 180 ° rotationally symmetric arrangement is employed. It is not limited to such a configuration. The configuration in the eighth and ninth embodiments is applied to one of the pair of ultrasonic transducers, and a different configuration (for example, the configuration shown in FIGS. 15A to 15C) is applied to the other ultrasonic transducer. Is also good. In the eighth and ninth embodiments, the ultrasonic transducer is used as the ultrasonic transducer, Force for Performing Reception as well as Transmission of Ultrasonic Waves The eighth and ninth embodiments of the present invention are not limited to such a configuration. Separate ultrasonic transducers may be used for transmission and reception.

According to the eighth and ninth embodiments of the present invention, since the loss when propagating the ultrasonic wave into the measured flow rate can be reduced to almost zero, the flow rates of various fluids including gas can be controlled with high sensitivity. Can be measured.

Also, according to the eighth and ninth embodiments of the present invention, it is not necessary to provide steps or irregularities inside the flow path, so that it is possible to measure a very small flow rate without disturbing the flow of the fluid to be measured. .

According to the present invention, an ultrasonic transmission / reception unit that transmits and / or receives an ultrasonic wave, and a propagation medium portion that forms a propagation path of the ultrasonic wave, the density P and the sound velocity C of the propagation medium portion, and By properly setting the correlation between the density p ₂ and the sound velocity C ₂ of the fluid filling the surrounding space, and refracting the ultrasonic wave at an appropriate angle, the loss when radiating the ultrasound to the fluid filling the surrounding space is reduced. Efficient transmission / reception for various fluids including gas, since it can be reduced to almost zero and / or the loss when receiving ultrasonic waves from the fluid filling the surrounding space can be reduced to almost zero Becomes possible. When the fluid is a gas, it can transmit and receive almost horizontally (parallel) to the transmitting and receiving surface of the ultrasonic transmitter and receiver, and can be used for various applications.

Note that by appropriately combining any of the various embodiments described above, the effects of the respective embodiments can be achieved.

While the present invention has been fully described in connection with the preferred embodiments thereof with reference to the accompanying drawings, various changes and modifications will be apparent to those skilled in the art. It is to be understood that such changes and modifications are intended to be included therein without departing from the scope of the invention as set forth in the appended claims.

Claims

The scope of the claims

1. an ultrasonic sensor that transmits or receives ultrasonic waves to a surrounding space filled with fluid,

The ultrasonic transducer (2, 1, 2, 22, 32, 42, 52, 62, 72) and the space between the ultrasonic transducer and the surrounding space are filled and the propagation path of the ultrasonic wave is An ultrasonic sensor including a propagation medium portion (6, 6A, 6B, 6C, 6D, 6E, 6F, 6G) to be formed.

2. An ultrasonic sensor that transmits or receives ultrasonic waves to a surrounding space filled with fluid,

The ultrasonic transducer (2, 12, 22, 22, 32, 42, 52, 62, 72) is disposed between the ultrasonic transducer and the surrounding space, and forms the propagation path of the ultrasonic wave. Propagation medium part (6, 6A, 6B, 6C, 6D, 6E, 6F, 6G)

The density p of the propagation medium part is the sound velocity C of the propagation medium part, and the density p _{2 of} the fluid filling the space and the sound velocity C _{2 of the} fluid filling the space are (p ₂ / _P

,) <{c c ^ An ultrasonic sensor configured to satisfy the relationship of 1.

3. The propagation medium portion has a first surface region (7) facing the ultrasonic vibration surface of the ultrasonic vibrator and a second surface region (8) facing the flow filling the surrounding space. 3. The ultrasonic sensor according to claim 2, wherein the second surface region of the propagation medium portion is inclined with respect to the first surface region.

4. An ultrasonic sensor that transmits or receives ultrasonic waves to a surrounding space filled with fluid,

Ultrasonic transducers (42, 52, 62, 72),

A propagation medium (6D, 6E, 6F, 6G) that is disposed between the ultrasonic transducer and the surrounding space and that forms a propagation path of the ultrasonic wave;

A reflector (44, 54, 64, 74) that is disposed in contact with the propagation medium and controls the propagation path of the ultrasonic wave;

Density of the propagation medium part P Sound velocity in the propagation medium part C An ultrasonic sensor configured so that the density p _{2 of} the fluid to be added and the sound speed C _{2 of the} fluid filling the space satisfy the relationship of (p ₂ / p × ic c ₂ ) <1.

5. The propagation medium portion includes a first surface region (7) facing the ultrasonic vibration surface of the ultrasonic vibrator, a second surface region (8) facing the flow filling the surrounding space, And having at least one third surface region (45, 55) disposed between the first surface region and the second surface region of the ultrasonic wave propagation path and in contact with the reflector; 5. The ultrasonic sensor according to claim 4, wherein the second surface region of the propagation medium section is inclined with respect to at least one of the first surface region and the third surface region.

6. The density p _{τ of} the propagation medium, the angle of incidence of ultrasonic waves at the interface between the propagation medium and the fluid filling the surrounding space, and the density ρ _{2 of} the fluid filling the surrounding space, and The angle of incidence of the ultrasonic wave from the interface to the fluid filling the surrounding space, 0 _2, is configured to substantially satisfy the relationship ρ ₂ / _{P l} = cot Θ ₂ / cot Θ. Ultrasonic sensor according to one.

7. The ultrasonic sensor according to claim 1, wherein the propagation medium portion is formed from a dried gel of an inorganic oxide or an organic polymer.

8. The ultrasonic transmission sensor according to claim 6, wherein the solid skeleton of the dried gel is hydrophobized.

9 · The ultrasonic sensor according to claim 7, wherein the density of the dried gel is 500 kg Zm ³ or less, and the average pore diameter of the dried gel is 100 nm or less.

10. An acoustic matching layer provided between the ultrasonic vibrator and the propagation medium part for acoustically matching the ultrasonic vibrator and the propagation medium part. The ultrasonic sensor according to any one of claims 1 to 5, wherein the ultrasonic sensor has (33), (43), (53), (63), (73).

Ultrasonic sensor according to 1 1. fluid filling the surrounding space, any one of claims 1-5 density p ₂ is 1 0 kg Zm ³ following gases.

1 2. The ultrasonic sensor according to any one of claims 1 to 5, wherein a transmitting or receiving direction of the ultrasonic wave is substantially parallel to the second surface region.

1 3. A flow measuring unit (304) having an inner wall that defines the flow path of the fluid to be measured; At least one ultrasonic vibrator (301 a, 30) that is provided outside the flow path space (309) surrounded by the inner wall (340) of the flow rate measuring unit and transmits or receives ultrasonic waves. 1 b) and

A propagation medium portion (303a, 303b) that is disposed between the ultrasonic transducer and the flow path space and that forms the ultrasonic wave propagation path;

An ultrasonic flowmeter having

The density _{P of the} propagation medium part, the sound velocity C in the propagation medium part, the density p _{2 of} the measured fluid, and the sound velocity c _{2 of the} measured fluid are (p ₂ p) <(cc ₂ ) <ι. An ultrasonic flowmeter configured to satisfy the above relationship.

1 4. The number of ultrasonic transducers is more than one,

A first ultrasonic transducer of the plurality of ultrasonic transducers is arranged to emit an ultrasonic wave to a second ultrasonic transducer of the plurality of ultrasonic transducers, 14. The ultrasonic flowmeter according to claim 13, wherein the second ultrasonic vibrator is arranged to emit an ultrasonic wave to the first ultrasonic vibrator.

1 5. The propagation medium portion has a first surface region (3 3 1) facing the ultrasonic vibration surface of the ultrasonic vibrator and a second surface region (3 3 2) facing the flow path space. And has

15. The ultrasonic flowmeter according to claim 13, wherein the second surface region of the propagation medium portion is inclined with respect to the first surface region.

1 6. The first surface region of the propagation medium portion is inclined with respect to the flow direction of the fluid to be measured in the flow path space, and the second surface region is inclined in the flow path space. 16. The ultrasonic flowmeter according to claim 15, wherein the ultrasonic flowmeter is parallel to a flow direction of the fluid to be measured.

17. The ultrasonic flowmeter according to claim 15, wherein the second surface region of the propagation medium section does not substantially form a step with the inner wall of the flow rate measurement section.

1 8. Density p J of the propagation medium part, angle of incidence of ultrasonic waves on the interface between the propagation medium part and the fluid to be measuredΘ Density p _{2 of} the fluid to be measured, and the above from the interface The penetration angle θ _{2 of the} ultrasonic wave into the fluid to be measured is

_{_{p 2 / P l = cot 0}} 2 / claim configured to satisfy approximately the relation cot 0 An ultrasonic flowmeter according to any one of 13 to 16.

1 9. the fluid to be measured, an ultrasonic flowmeter according to claim 1 3-1 6 density p ₂ is 10 kg · ^m-3 or less gas.

20. The ultrasonic flowmeter according to any one of claims 13 to 16, wherein the propagation medium portion is formed from a dried gel of an inorganic oxide or an organic polymer.

21. The ultrasonic flowmeter according to claim 20, wherein the solid skeleton of the dried gel is hydrophobized.

22. The density of the dry gel is at 500 kg / m ³ or less,

22. The ultrasonic flowmeter according to claim 21, wherein the average pore diameter of the dried gel is 100 nm or less.

23. A matching layer provided between the ultrasonic vibrator and the propagation medium portion, the matching layer acoustically matching the ultrasonic vibrator and the propagation medium portion. 7. The ultrasonic flowmeter according to any one of 6.

24. The size of the flow path space in the flow velocity measuring unit measured in a direction perpendicular to the flow velocity direction of the fluid to be measured is not more than 1/2 of the wavelength in the fluid to be measured at the center frequency of the ultrasonic wave. The ultrasonic flowmeter according to any one of claims 13 to 16.

2 5. The ultrasonic flowmeter according to claim 13, wherein the ultrasonic vibrator forms a convergent sound field.

26. The ultrasonic flowmeter according to claim 24, wherein the first surface region of the propagation medium portion (308a, 308b) is curved to form a lens surface.

2 7. A flow measurement unit (304) having an inner wall that defines a gas flow path and an outside of a flow path space (309) surrounded by the inner wall (340) of the flow measurement unit, transmitting ultrasonic waves. Or a pair of ultrasonic transducers (30 1 a, 301 b) for receiving,

A pair of propagation medium portions (303a, 303b) disposed between each of the pair of ultrasonic transducers and the flow path space and refracting a propagation path of the ultrasonic wave;

With

The propagation medium portion has a first surface area (331) facing the ultrasonic vibration surface of the ultrasonic vibrator and a second surface area (332) facing the flow path space. , The first surface region of the propagation medium portion is inclined with respect to the flow direction of the gas in the flow path space, and the second surface region is inclined with respect to the flow direction of the gas in the flow path space. Ultrasonic flow meter that is almost parallel.

28. The ultrasonic flowmeter according to any one of claims 13 to 16,

A pipe (304) for supplying a fluid to be measured to the ultrasonic flowmeter,

A display unit (703) for displaying a flow rate measured by the ultrasonic flowmeter.

29. An ultrasonic sensor for transmitting or receiving ultrasonic waves to or from a surrounding space filled with fluid,

The ultrasonic transducer (2, 12, 22, 32, 42, 52, 62, 72) and the space between the ultrasonic transducer and the surrounding space are filled to form a propagation path of the ultrasonic wave Propagation medium part (6, 6 A, 6B, 6C, 6D, 6E, 6F, 6 G)

The propagation medium portion has a first surface region (7) facing the ultrasonic vibration surface of the ultrasonic transducer and a second surface region (8) facing a flow that fills the surrounding space. An ultrasonic sensor, wherein the second surface region of the propagation medium portion is inclined with respect to the first surface region.